BACKGROUND OF THE INVENTION
I. Field Of The Invention
[0001] This invention relates to optical communication systems. More particularly, the invention
is directed to lasers used in optical communication systems for providing electromagnetic
energy at many different frequencies.
II. Background Art
[0002] High capacity optical communication systems require that many optical signals be
frequency division multiplexed in the components of an optical network. This requires
that there be a way of conveniently producing electromagnetic energy at many different
frequencies. An ideal device for producing optical energy useful in an optical communication
system is a laser. Recently, such lasers have been constructed as substrates or wafers
comprised of semiconductor material having a frequency router connected to active
sections, comprised of optical amplifiers, and selective sections, also comprised
of optical amplifiers. A laser of this type is for example disclosed in EP-A-0 612
125, and is depicted in FIG. 1 of the drawings.
[0003] The laser 5 of FIG. 1 is seen to include a substrate or wafer 10 having a first cleaved
face 20 and a second cleaved face 24, and formed in a manner well known to those of
ordinary skill in the art. An NxN frequency routing device 12 is formed in the wafer
10 between the faces 20 and 24. One side of the laser 5 -- the left side in FIG. 1
-- is formed of a plurality of active optical amplifiers defining active sections
18₁ through 18
N, each in contact with a corresponding waveguide in a first plurality of waveguides
14₁ through 14
N. The waveguides are, in turn, connected to the left side of the frequency router
12. For lasing, one of the optical amplifiers 18 (such as the optical amplifier 18₁
in FIG. 1) is DC biased in its active region so as to become light-transmissive and
to provide gain to the selected lased frequencies, as more fully explained below.
[0004] The other side of laser 5 -- the right side in FIG. 1 -- has a plurality of selectively
activatable optical amplifiers or gates 22₁ through 22
N which are placed at the second cleaved face 24 for forming a lasing path through
which lasing occurs. Each selectively activatable optical amplifier 22 is connected
to a corresponding one of the plurality of waveguides 16₁ through 16
N which are connected to the frequency router 12, i.e. to the left side of the router
12 in FIG. 1. The laser 5 is operated by forming lasing paths between one of the waveguides
14 which are connected to a corresponding active optical amplifier 18, and one or
more of the waveguides 16 which are connected to the corresponding selectively activatable
optical amplifiers 22.
[0005] Each optical amplifier comprises a doped section having controllable optical transmissivity.
The doping level is such that an appropriately configured semiconductor junction is
defined in each optical amplifier. These doped sections are optically active in that
an application of electrical energy to those sections will cause them to become transmissive
to the flow of optical energy and will even provide some degree of gain to optical
signals flowing through them. When electrical bias current above a lasing threshold
is applied, laser action begins. The doped sections are substantially opaque to the
transmission of light when no electrical stimulation is applied. However, when electrical
stimulation is applied, these sections become light transmissive. Thus, for example,
a lasing path is created by applying the appropriate electrical stimulation, i.e.
an amount above the lasing threshold, to optical amplifier 18 and to any of the selectively
activatable optical amplifiers such as the amplifiers 22₃ and 22₆.
[0006] The frequency router 12 is a bidirectional device capable of multiplexing and demultiplexing
optical signals and also possesses a wraparound feature. For an optical signal having
a frequency F₁ appearing on waveguide 14₁ and flowing toward the router 12, the signal
will be directed to the waveguide 16₁. Conversely, an optical signal having a frequency
F₁ directed toward the router 12 on waveguide 16₁ will be directed by the router to
the waveguide 14₁. An optical signal having a frequency F₂ appearing on waveguide
14₁ and flowing toward the router 12 will be directed to the waveguide 16₂ and an
optical signal having a frequency F₂ directed toward the router 12 on waveguide 16₂
will be directed toward guide 14₁. Thus, by way of illustration, for a four port frequency
router 12 having a signal F comprised of four discrete frequency components F₁, F₂,
F₃ and F₄ appearing on waveguide 14₁, the router 12 will demultiplex and direct the
individual frequency components to waveguides 16 such that component F₁ appears at
waveguide 16₁, component F₂ appears at waveguide 16₂, etc.
[0007] In addition and as stated above, the router 12 contains a wraparound feature which
is inherent to the device. Thus, for a signal F having discrete frequency components
F₁, F₂, F₃ and F₄ appearing on waveguide 14₂ and flowing toward the router 12, the
components will be directed to waveguides 16 such that frequency component F₁ appears
at waveguide 16₂, frequency component F₂ appears at waveguide 16₃, frequency component
F₃ appears at waveguide 16₄ and frequency component F₄ appears at waveguide 16₁. In
other words, if the signal F appears at a waveguide 14₂ which provides the signal
to the router one waveguide position below the position of waveguide 14₁, each frequency
component appears at a correspondingly shifted waveguide. In this example, the described
router 12 contains only four waveguides 16₁ through 16₄. Thus, frequency component
F₄ is wrapped around and routed to waveguide 16₁.
[0008] When optical amplifier 22₃ is activated by applying thereto an appropriate DC bias
voltage, lasing at a frequency F₃ occurs through the lasing path defined by waveguide
16₃, frequency router 12 and waveguide 14. The laser 5 is capable of operating at
two or more simultaneous frequencies and generates a multiplexed output made up of
the lased signals. Thus, as seen in FIG. 1, gate 22₆ is also activated which generates
lasing at frequency F₆ through a lasing path defined by waveguide 16₆, frequency router
12, and waveguide 14₁. The output signal accordingly contains frequencies F₃ and F₆.
In operation, each frequency is modulated at a distinct rate (identified as M₁ and
M₂ in FIG. 1), to provide data to the lased frequencies (F₃ and F₆), which data can
be retrieved through known demodulation techniques.
[0009] While the prior art laser 5 of FIG. 1 is useful in optical communication systems
because it is capable of operating at two or more simultaneous frequencies and generating
a multiplexed output comprised of the multiple lased frequencies, the laser is nonetheless
limited in several important respects. First, when such a laser is operated at two
or more simultaneous frequencies, the output contains readily perceivable crosstalk.
Second, because the modulation rate is related to the length of the lasing cavity,
for the laser depicted in FIG. 1 the modulation rate is limited to about 150 Mb/s
due to the relatively large size of the lasing path. This, of course, limits the amount
of data that each frequency is capable of carrying. Thus, it would be desirable to
have a digitally-tuned laser that is capable of operating at two or more simultaneous
frequencies while eliminating crosstalk and appreciably increasing the attainable
modulation rate.
SUMMARY OF THE INVENTION
[0010] The present invention is accordingly directed to a digitally-tuned integrated laser
with multi-frequency operation. The laser comprises a wafer having a frequency router
disposed between a first cleaved face and a second cleaved face and which defines
a laser cavity. An active optical amplifier is formed at the first cleaved face for
operation in an active mode. A waveguide connects the active optical amplifier to
the frequency router.
[0011] The laser also includes a plurality of pairs of selectively activated optical amplifiers
formed at the second cleaved face. Each pair of selectively activated amplifiers has
a first and a second optical amplifier, the second amplifier of each pair being selectively
activatable by a control signal. A plurality of waveguide pairs, each pair comprising
first and second waveguides, are connected to the selectively activated amplifiers
so that the second waveguide of each pair is connected to the corresponding second
optical amplifier, thereby defining a lasing path for the generated signal, and the
first waveguide of each pair is connected to the corresponding first optical amplifier.
Means for optically coupling a respective first waveguide of each waveguide pair to
its corresponding second waveguide are provided for splitting the selected lasing
frequency into first and second portions with the first portions being directed to
corresponding first waveguides of the waveguide pairs and the second portions being
directed to corresponding second waveguides of the waveguide pairs. Means are also
provided for modulating the first portions of the selected lasing frequency and then
providing the modulated portions to the frequency router which directs the modulated
portions to an output port.
[0012] Other objects and features of the present invention will become apparent from the
following detailed description considered in conjunction with the accompanying drawings.
It is to be understood, however, that the drawings are designed solely for purposes
of illustration and not as a definition of the limits of the invention, for which
reference should be made to the appended claims.
BRIEF DESCRIPTION OF THE DRAWINGS
[0013] In the drawings, wherein like reference characters denote similar elements throughout
the several views:
FIG. 1 is a block schematic diagram of a prior art digitally-tuned laser; and
FIG. 2 is a block schematic diagram of an improved digitally-tuned laser constructed
in accordance with the teachings of the present invention.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
[0014] FIG. 2 of the drawings depicts an improved digitally-tuned laser 5' with multi-frequency
operation that is constructed in accordance with the present invention. The laser
5', like the prior art laser 5 of FIG. 1, is formed in a substrate or wafer 10 having
a first cleaved face 20 and a second cleaved face 24, and further includes a third
face 11 which is preferably substantially perpendicular to the cleaved faces 20 and
24. As explained above, in respect of the prior art construction, for lasing to occur
only one of the amplifiers 18 of FIG. 1 is biased in the active mode. For this reason,
FIG. 2 depicts a single optical amplifier 18 which is disposed at or proximate the
first cleaved face 20. Optical amplifier 18 is connected to a corresponding waveguide
14 which, in turn, is connected to a 2x2N frequency router 12. An additional waveguide
13 is also included which is connected to frequency router 12. As in the prior art
laser of FIG. 1, the optical amplifier 18 restricts the flow of optical energy, or
light, when biased below a threshold lasing voltage and allows the flow of optical
energy when biased above the threshold lasing voltage.
[0015] Unlike that of the prior art laser 5, the right side of the inventive laser 5' depicted
in FIG. 2 includes a plurality of pairs of optical amplifiers or gates 22, with each
pair comprising a modulated path optical amplifier 22₁' through 22
N' and a selectively activatable optical amplifier or gate 22₁ through 22
N. Thus, the first pair of optical amplifiers is formed of the selectively activatable
gate 22₁ and the modulated path amplifier 22₁', the second pair is formed of the selectively
activatable gate 22₂ and modulated path amplifier 22₂', and so on. Each gate 22 is
connected to a corresponding waveguide 16₁ through 16
N which collectively form a plurality of waveguides, and each modulated path optical
amplifier 22' is connected to a corresponding modulated waveguide 16₁' through 16
N' which likewise form a plurality of modulated waveguides, as shown in FIG. 2.
[0016] Each selectively activatable optical amplifier or gate 22₁ through 22
N is responsive to a control signal generated from a gate control circuit 30 for selecting
which of the gates 22₁ through 22
N is to be activated, thereby determining at which frequency lasing will occur. As
the gates are only light transmissive when biased in an active mode, i.e. when a control
signal exceeding the lasing threshold is applied, and because amplifier 18 is always
biased in the active mode, lasing will occur at a particular frequency when the corresponding
gate is selected by the gate control circuit 30. Thus, if gate 22₃ is activated, a
lasing path defined by waveguide 16₃, router 12 and waveguide 14 is formed and lasing
occurs at frequency F₃.
[0017] With continued reference to FIG. 2, each modulated waveguide 16' comprises an optical
coupler 28 and a modulator 26. The optical coupler joins each modulated waveguide
16' to its corresponding waveguide 16. Thus, optical coupler 28₁ couples waveguide
16₁ to modulated waveguide 16₁', optical coupler 28₂ couples waveguide 16₂ to modulated
waveguide 16₂', and so on. The modulator 26 of each modulated waveguide 16' is disposed
in-line with the modulated waveguide 16' to modulate a portion of the selected lasing
frequency, as more fully described below. Also as shown, the signal on the modulated
waveguide 16' is supplied to the frequency router 12 at a port different than the
port connected to the waveguide 16.
[0018] To produce laser light at one of N discrete frequencies, such for example as the
frequencies F₃ and F₆ in FIG. 2, the gate control circuit 30 supplies a control signal
in the form of a bias current to gates 22₃ and 22₆. This activates the lasing paths
through which laser light having frequencies F₃ and F₆ are generated, resulting in
a lasing path for frequency F₆ between gate 22₆ and active optical amplifier 18, and
a lasing path for frequency F₃ between gate 22₃ and active optical amplifier 18.
[0019] When gates 22₃ and 22₆ are activated by the control signal from circuit 30, the optical
couplers 28₃ and 28₆ respectively connected thereto split a portion of the signal
on the corresponding waveguides 16₃ and 16₆ and direct them to the corresponding modulators
26₃ and 26₆ which modulate the signal at a predetermined rate and provide the so modulated
signals to the frequency router 12 via modulated waveguides 16₃' and 16₆'. Thus, optical
coupler 28₃ splits a portion of the optical signal having frequency F₃, which is then
modulated at a rate of M₃ by modulator 26₃ and supplied to the frequency router 12
via modulated input waveguide 16₃'. The modulated frequency is depicted in FIG. 2
as the broken or dashed line F₃'. A like process occurs for the optical signal of
frequency F₆. In other words, the signal F₆ is coupled via optical coupler 28₆, is
modulated at a rate of M₆ by modulator 26₆ and is supplied to frequency router 12.
The modulated frequency F₆ is depicted in FIG. 2 as the broken or dashed line F₆'.
[0020] As mentioned above, since the modulated signals are supplied to the frequency router
12 one port position above the unmodulated signals, the modulated multiplexed signal
comprised of the selected modulated discrete frequency components is likewise directed
to waveguide 13 which is different and, in fact, one port above the waveguide containing
the unmodulated signals; i.e. waveguide 14. In the preferred embodiment, the waveguide
13 is combined and/or oriented to direct the generated signal to the third face 11
of wafer 10, which face 11 is coated with an anti-reflection material to further maximize
the output signal. In addition, as the unmodulated signal is no longer needed, the
cleaved faces 22 and 24 are coated with a high reflection material to prevent or impede
passage of the unmodulated optical signals. It is also noted that as the modulated
path optical amplifiers 22' are not operated in the active mode and are therefore
light absorptive, these amplifiers reduce degenerative feedback in the laser 5' because
the amplifiers 22' absorb the portions of the optical signals which may be fed back
through the optical couplers 28.
[0021] As will now be appreciated, the laser 5' of the present invention does not modulate
the generated lased optical signals within the lasing path (as in the prior art arrangement
of in FIG. 1) but, instead, operatively employs a plurality of internal modulators
26 formed on the wafer 10 for modulating a portion of the lased signal outside of
the lasing path. As such, the limiting relationship between the modulation rate and
the length of the lasing cavity in prior art digitally-tuned lasers is not present
in lasers constructed in accordance with the present invention, thereby permitting
the realization and use of faster modulation rates. In addition, the laser configuration
of the present invention eliminates the crosstalk that was present when the prior
art laser of FIG. 1 was operated at two or more simultaneous frequencies.
[0022] While there have been shown and described and pointed out fundamental novel features
of the invention as applied to a currently preferred embodiment thereof, it will be
understood that various omissions and substitutions and changes in the form and details
of the apparatus illustrated, and in its operation, may be made by those skilled in
the art without departing from the invention. It is the intention, therefore, to be
limited only as indicated by the scope of the claims appended hereto.
1. A digitally-tuned integrated laser with multi-frequency operation for generating an
optical signal, said laser comprising:
a wafer having a first cleaved face and a second cleaved face for defining a laser
cavity:
a frequency router formed in said wafer;
an optical amplifier formed at said first cleaved face for operation in an active
mode;
a first pair of waveguides comprising a first waveguide and a second waveguide,
said second waveguide connecting said optical amplifier to said frequency router;
a pair of optical amplifiers formed at said second cleaved face, said pair comprising
first and second optical amplifiers, said second amplifier being selectively activatable
by a control signal;
a second pair of waveguides comprising a first waveguide and a second waveguide,
said second waveguide being connected to said second optical amplifier, thereby defining
a lasing path for the generated optical signal;
means for optically coupling the first waveguide of said second pair of waveguides
to the second waveguide of said second pair of waveguides for splitting the generated
optical signal into first and second portions respectively directed to said first
and second waveguides in said second pair of waveguides so as to provide paths between
said optical amplifier pair and said frequency router for the first and second portion
of said generated optical signal for applying the first and second portions of the
generated optical signal to said frequency router; and
means for modulating said first portion of the optical signal before said portion
is applied to said router, to define a modulated first portion of the generated optical
signal which is directed to said first waveguide of said first pair of waveguides
by said frequency router.
2. The laser of claim 1, wherein said wafer further comprises a third face substantially
parallel to said second cleaved face, and wherein said first waveguide of said first
pair of waveguides connects said third face to said frequency router.
3. The laser of claim 2, wherein said first and second cleaved faces are coated with
a high reflection material and wherein said third face is coated with an anti-reflection
material.
4. A digitally-tuned integrated laser with multi-frequency operation for generating optical
signals of various frequencies, said laser comprising:
a wafer having a first cleaved face and a second cleaved face for defining a laser
cavity:
a frequency router formed in said wafer;
an optical amplifier formed at said first cleaved face for operation in an active
mode;
a pair of waveguides comprising a first waveguide and a second waveguide, said
second waveguide connecting said optical amplifier to said frequency router;
a plurality of pairs of optical amplifiers formed at said second cleaved face,
each said pair comprising first and second optical amplifiers, and said second amplifiers
of each said pair being selectively activatable by a control signal;
a plurality of waveguide pairs, each said waveguide pair comprising a first waveguide
and a second waveguide, said second waveguide of each said waveguide pair being connected
to a corresponding one of said second optical amplifiers, thereby defining a lasing
path for the generated optical signals;
means for optically coupling the first waveguide of each said waveguide pair to
said second waveguide of said each said waveguide pair for splitting the generated
optical signals into first and second portions respectively directed to said corresponding
first and second waveguides of said each said waveguide pair so as to provide paths
for the first and second portions of said generated optical signals between said plurality
of optical amplifier pairs and said frequency router for applying the first and second
portions of the generated optical signals to said frequency router; and
means for modulating said first portions of said generated optical signals before
said portions are applied to said frequency router to define modulated first portions
of said generated optical signal which are directed to said first waveguide of said
pair of waveguides by said frequency router.
5. The laser of claim 4, wherein said wafer further comprises a third face substantially
parallel to said second cleaved face, and wherein said first waveguide of said pair
of waveguides connects said third face to said frequency router.
6. The laser of claim 5, wherein said first and second cleaved faces are coated with
a high reflection material and wherein said third face is coated with an anti-reflection
material.